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211.
A. Chatterjee B. K. Chakrabarti 《The European Physical Journal B - Condensed Matter and Complex Systems》2006,54(3):399-404
We study here numerically the behavior of an ideal gas like model of markets having
only one non-consumable commodity. We investigate the behavior of the
steady-state distributions of money, commodity and total wealth,
as the dynamics of trading or exchange of money and commodity proceeds,
with local (in time) fluctuations in the price of the commodity.
These distributions are studied in markets with agents having uniform and
random saving factors. The self-organizing features in money distribution
are similar to the cases without any commodity (or with consumable
commodities), while the commodity distribution shows an exponential decay.
The wealth distribution shows interesting behavior: gamma like
distribution for uniform saving propensity and has the same power-law tail,
as that of the money distribution, for
a market with agents having random saving propensity. 相似文献
212.
C. Bai Y. -L. Yang X. -D. Zhang 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,65(1):79-84
Based on the extended Blonder-Tinkham-Klapwijk (BTK) approach, we have investigated the coherent quantum transport in two-dimensional
electron gas/superconductor (2DEG/SC) double tunneling junctions in the presence of the Rashba spin-orbit coupling (RSOC).
It is found that all the reflection coefficients in BTK theory as well as conductance spectra oscillate with the external
voltage and energy. The oscillation feature of conductance can be tuned largely by the RSOC for low insulating barriers, while
for high insulating barriers it is almost independent of the RSOC. These phenomena are essentially different from those found
in ferromagnet/superconductor double tunneling junctions. 相似文献
213.
Sumana Chakraborty Yew Kam Ho 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,49(1):59-65
This work presents an investigation on the doubly excited 1S
e
autoionizing states of screened helium atom lying below the n = 4 threshold of the He+ ion. The potential generated in this system is represented by a Yukawa type potential. We have employed complex-coordinate
rotation method, as it is a powerful scheme to study high lying resonances. Hylleraas type wave function is used to consider
the correlation effect between all the charged particles. Our resonance parameters for the resonances lying below the He+ (n = 2) threshold agree well with those of the existing calculations by using the stabilization method. Resonances associated
with higher thresholds are new calculations. All the present results are well converged with basis length N = 444. 相似文献
214.
B. G. Bhaskaran 《Queueing Systems》1986,1(1):103-127
Given conditions, which concern the infinitesimal parameters of two birth and death processes, the processes are constructed on the same probability space such that one process is almost surely larger than the other. Application is made to M/M/s queueing systems. Stochastic comparisons of queue length and virtual waiting time in two M/M/s systems are obtained. 相似文献
215.
本文对三阶非线性极化率的多种测量方法进行了比较研究,分析了每种方法的优缺点,对于实际情况下各类光学材料非线性性质的测量具有一定的指导意义。 相似文献
216.
217.
对MMC微裂纹分布的SEM照片连续地变换网格尺度,求得了MMC微裂纹分布的自相似分形维数,D=1.56.对大塑性变形后MMC分形重建后的σ(t)时间序列进行了非线性动力学过程分析,找到了相空间吸引子积分关联函数,确定了该MMC微裂纹演化存在吸引子,其分形关联维数值1.48与实验测得自相似分形维数值1.56接近。 相似文献
218.
The upper estimates of the functions that satisfy some differential integral inequality are established in this paper. We obtain the uniform estimates of maximum of the solutions for a general class of parabolic equations and extend some known results. 相似文献
219.
In this paper,we study the surface instability of a cylindrical pore in the absence of stress. This instability is called the Rayleigh-Plateau instabilty. We consider the model developed by Spencer et ... 相似文献
220.
级联二阶非线性法布里-珀罗谐振腔特性分析 总被引:1,自引:0,他引:1
在小信号近似下,得出了级联二阶过程的表达式。利用该式的有效三阶极化率的表达式,讨论了存在二阶非线性光学晶体的法-珀谐振腔的非线性光学特性。分析表明,由于谐振腔的存在,通过非线性晶体的功率密度超过入射功率密度几十倍以上,因而产生较大的、随相位失配变化的非线性相位漂移。当相位失配接近2π时,获得基叔光的最大相位漂移。该最大相位漂移对应的相位失配随着入射功率密度、非线性晶体的地阶极化率和晶体长度而变化。 相似文献